A formalism for treating the scattering of decuplet baryons in chiral effective field theory is developed. The minimal Lagrangian and potentials in leading-order SU(3) chiral effective field theory for the interactions of octet baryons (B) and decuplet baryons (D) for the transitions BB → BB, BB ↔ DB, DB → DB, BB ↔ DD, DB ↔ DD, and DD → DD are provided. As an application of the formalism we compare with results from lattice QCD simulations for ΩΩ and N Ω scattering. Implications of our results pertinent to the quest for dibaryons are discussed.